2019
DOI: 10.1088/1475-7516/2019/07/030
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Relativistic cosmological large scale structures at one-loop

Abstract: The large scale structure bispectrum in the squeezed limit couples large with small scales. Since relativity is important at large scales and non-linear loop corrections are important at small scales, the proper calculation of the observed bispectrum in this limit requires a non-linear relativistic calculation. We compute the matter bispectrum in general relativity in the weak field approximation. The calculation is as involved as existing second-order results. We find several differences with the Newtonian ca… Show more

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Cited by 32 publications
(60 citation statements)
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“…These become important when probing the largest scales of the galaxy power spectrum, where the imprint of sizable primordial bispectra in the squeezed configuration is strongest. Several analyses have computed these corrections [234,282,[353][354][355][356][357][358][359][360] and the importance of these relativistic corrections has been quantified for forthcoming surveys [361][362][363].…”
Section: Observational Prospectsmentioning
confidence: 99%
“…These become important when probing the largest scales of the galaxy power spectrum, where the imprint of sizable primordial bispectra in the squeezed configuration is strongest. Several analyses have computed these corrections [234,282,[353][354][355][356][357][358][359][360] and the importance of these relativistic corrections has been quantified for forthcoming surveys [361][362][363].…”
Section: Observational Prospectsmentioning
confidence: 99%
“…Let us point out that we will consider the Newtonian kernels [30,31] in the rest of the paper, which is in line with neglecting terms of higher order in H/k, see [32]. Our results can be generalized to an arbitrary (separable) non-linear velocity kernel G 2 (k 1 , k 2 ), including the full higher order GR dynamics [32][33][34][35].…”
Section: Rsd Hmentioning
confidence: 57%
“…More generally, the extension of the techniques described in this paper to include mixedorder quantities like δ (1,1) and post-Newtonian quantities like δ (0,4) is conceivable, as is modifying the NPT sector to incorporate the renormalised perturbation theory of Crocce and Scoccimaro [50] or the EFTofLSS [10]. Comparison to analytic weak-field results like those in [25] and to simulations like gevolution [51] may yield insight into both the nature of twoparameter perturbation theory, but also to weak-field general relativity, a scheme close in spirit to that of two-parameter perturbation theory. In particular, it may be necessary to renormalize the background quantities as is done in Ref.…”
Section: Discussionmentioning
confidence: 92%
“…where φ (2) 0 can be obtained from ψ (2) 0 using the constraint from Equation (5. 25), and Ψ 0 is the quantity defined in Eq. (4.20) .…”
Section: Evolution Of Gravitational Potentials In 2pptmentioning
confidence: 99%